235 research outputs found
Subcortical brain atrophy persists even in HAART-regulated HIV disease
- Author
- A Antinori
- AA Moeller
- Ann Ragin
- Bruce Cohen
- CA Wiley
- CJ Holmes
- CM Marra
- CM Marra
- EA Childs
- Eileen Martin
- Eric N. Miller
- G Fagiolo
- HS Levin
- James T. Becker
- JC Stout
- Jeffery R. Alger
- JG Dal Pan
- JJ Lin
- JM Castelo
- Joanne Sanders
- JR Berger
- JR Berger
- JT Becker
- K Hestad
- K Kieburtz
- Karl Goodkin
- L Chang
- L Chang
- LA Cysique
- LA Cysique
- LA Kingsley
- LAJ Cysique
- Lawrence Kingsley
- MC Chiang
- MC Marcondes
- N Lepore
- Ned Sacktor
- OT Carmichael
- OT Carmichael
- Owen T. Carmichael
- Paul M. Thompson
- Peter B. Barker
- PM Thompson
- PM Thompson
- Priyanka Saharan
- RA Cohen
- RH Paul
- S Letendre
- Sarah K. Madsen
- T Ernst
- Victoria Maruca
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
The purpose of this study was to determine the pattern and extent of caudate nucleus and putamen atrophy in HIV-infected men with well-controlled immune status and viral replication. 155 men underwent structural brain magnetic resonance imaging; 84 were HIV-infected and 71 were uninfected controls. MRI data were processed using the Fully Deformable Segmentation routine, producing volumes for the right and left caudate nucleus and putamen, and 3-D maps of spatial patterns of thickness. There was significant atrophy in the HIV-infected men in both the caudate and putamen, principally in the anterior regions. The volume of the basal ganglia was inversely associated with the time since first seropositivity, suggesting that either there is a chronic, subclinical process that continues in spite of therapy, or that the extent of the initial insult caused the extent of atrophy
Measurement of the branching fraction and CP content for the decay B(0) -> D(*+)D(*-)
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Angelini C
- Anjomshoaa A
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Bellodi G
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bevan AJ
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Bucci F
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagna E
- Campagnari C
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davis CL
- De Groot N
- De Nardo G
- de Sangro R
- de Vaissiere C
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dittongo S
- Dixon P
- Dong D
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Grauges E
- Green MG
- Gritsan AV
- Grosdidier G
- Grothe M
- Groysman Y
- Guo QH
- Haas T
- Haire M
- Halyo V
- Hamilton R
- Hamon O
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson JR
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VB
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Marchiori G
- Margoni M
- Marker CE
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Monchenault GH
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Morton GW
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Pivk M
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roy J
- Ryd A
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott IJ
- Seiden A
- Sekula SJ
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yi J
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zallo A
- Zghiche A
- Zhang J
- Zhang L
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APS.We report a measurement of the branching fraction of the decay B0→D*+D*- and of the CP-odd component of its final state using the BABAR detector. With data corresponding to an integrated luminosity of 20.4 fb-1 collected at the Υ(4S) resonance during 1999–2000, we have reconstructed 38 candidate signal events in the mode B0→D*+D*- with an estimated background of 6.2±0.5 events. From these events, we determine the branching fraction to be B(B0→D*+D*-)=[8.3±1.6(stat)±1.2(syst)]×10-4. The measured CP-odd fraction of the final state is 0.22±0.18(stat)±0.03(syst).This work is supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the A.P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at √s=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Bright-Thomas PG
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bulos F
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Carroll M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark AR
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Copty N
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Coward DH
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Dauncey PD
- David P
- Davis CL
- De Groot N
- de la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dima MO
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Dyce N
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Fahey S
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Fullwood J
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- Geld TL
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Godfrey GL
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Green MG
- Grillo AA
- Gritsan AV
- Grosdidier G
- Grosso P
- Grothe M
- Groysman Y
- Gunawardane NJW
- Guo QH
- Haas T
- Haire M
- Hamilton R
- Hamon O
- Handler T
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson DR
- Johnson JR
- Johnson RP
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VG
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamanna E
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Leonardi E
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Margoni M
- Marker CE
- Marsiske H
- Martin JP
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazzoni MA
- McDonald KT
- McGrath P
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Moffeit KC
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Mount R
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Pia MG
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Rochester LS
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roussot E
- Roy J
- Ryd A
- Sadrozinski H
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott I
- Scott IJ
- Seiden A
- Seitz R
- Sekula SJ
- Sen S
- Serbo VV
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Simopoulos ET
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Smol A
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sutton CS
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qq̅ continuum events near the Υ(4S) resonance are presented. Using 20.8 fb-1 of data on the Υ(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(B⃗Ds+X)=(10.93±0.19±0.58±2.73)% and B(B⃗Ds*+X)=(7.9±0.8±0.7±2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+→φπ+ branching fraction uncertainty. The production cross sections σ(e+e-→Ds+X)×B(Ds+→φπ+)=7.55±0.20±0.34pb and σ(e+e-→Ds*±X)×B(Ds+→φπ+)=5.8±0.7±0.5pb are measured at center-of-mass energies about 40 MeV below the Υ(4S) mass. The branching fractions ΣB(B⃗Ds(*)+D(*))=(5.07±0.14±0.30±1.27)% and ΣB(B⃗Ds*+D(*))=(4.1±0.2±0.4±1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4±0.1±0.3MeV/c2 is also measured.This work was supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Multi-messenger observations of a binary neutron star merger
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- Zhang T
- Zhang W
- Zhang WC
- Zhang WZ
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
- Zhao HS
- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
- Zhou H
- Zhou J
- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zhu Y
- Zhu YX
- Zhu Z
- Ziegler A
- Zimmerman AB
- Zimmermann B
- Zimnukhov DS
- Ziolkowski M
- Zoll M
- Zong Z
- Zorn J
- Zornoza JD
- Zou CL
- Zuccarello F
- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Williams D
- Williamson Ar
- Willis Jl
- Willke B
- Winkler W
- Wipf Cc
- Wittel H
- Woan G
- Woehler J
- Wofford Jk
- Wright Jl
- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
- Yang Z
- Yap Mj
- Yazback M
- Yeeles Dw
- Yu H
- Yu Hc
- Yuen Shr
- Zadrozny A
- Zadrozny Ak
- Zanolin M
- Zelenova T
- Zendri Jp
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhao C
- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- College Park, MD : American Physical Society
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO's second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=3.47×10-25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering. © 2019 American Physical Society
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO’s second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h95%0=3.47×10−25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
- Author
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- Zhang Y-H
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- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17, the gravitational-wave event GW170817 was observed by the Advanced LIGO and Virgo detectors, and the gamma-ray burst (GRB) GRB 170817A was observed independently by the Fermi Gamma-ray Burst Monitor, and the Anti-Coincidence Shield for the Spectrometer for the International Gamma-Ray Astrophysics Laboratory. The probability of the near-simultaneous temporal and spatial observation of GRB 170817A and GW170817 occurring by chance is 5.0×10−8. We therefore confirm binary neutron star mergers as a progenitor of short GRBs. The association of GW170817 and GRB 170817A provides new insight into fundamental physics and the origin of short GRBs. We use the observed time delay of (+1.74±0.05)s between GRB 170817A and GW170817 to: (i) constrain the difference between the speed of gravity and the speed of light to be between −3×10−15 and +7×10−16 times the speed of light, (ii) place new bounds on the violation of Lorentz invariance, (iii) present a new test of the equivalence principle by constraining the Shapiro delay between gravitational and electromagnetic radiation. We also use the time delay to constrain the size and bulk Lorentz factor of the region emitting the gamma-rays. GRB 170817A is the closest short GRB with a known distance, but is between 2 and 6 orders of magnitude less energetic than other bursts with measured redshift. A new generation of gamma-ray detectors, and subthreshold searches in existing detectors, will be essential to detect similar short bursts at greater distances. Finally, we predict a joint detection rate for the Fermi Gamma-ray Burst Monitor and the Advanced LIGO and Virgo detectors of 0.1-1.4 per year during the 2018-2019 observing run and 0.3-1.7 per year at design sensitivity
Localization and broadband follow-up of the gravitational-wave transient GW150914
- Author
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- Zweizig J
- Publication venue
- Astrophysical Journal Letters
- Publication date
- 01/01/2016
- Field of study
A gravitational-wave (GW) transient was identified in data recorded by the Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) detectors on 2015 September 14. The event, initially designated G184098 and later given the name GW150914, is described in detail elsewhere. By prior arrangement, preliminary estimates of the time, significance, and sky location of the event were shared with 63 teams of observers covering radio, optical, near-infrared, X-ray, and gamma-ray wavelengths with ground- and space-based facilities. In this Letter we describe the low-latency analysis of the GW data and present the sky localization of the first observed compact binary merger. We summarize the follow-up observations reported by 25 teams via private Gamma-ray Coordinates Network circulars, giving an overview of the participating facilities, the GW sky localization coverage, the timeline, and depth of the observations. As this event turned out to be a binary black hole merger, there is little expectation of a detectable electromagnetic (EM) signature. Nevertheless, this first broadband campaign to search for a counterpart of an Advanced LIGO source represents a milestone and highlights the broad capabilities of the transient astronomy community and the observing strategies that have been developed to pursue neutron star binary merger events. Detailed investigations of the EM data and results of the EM follow-up campaign are being disseminated in papers by the individual teams
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Fiolhais MCN
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- Fleck I
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
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- Agaras MN
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- Aggarwal A
- Agheorghiesei C
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- Akolkar NN
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- Aleksa M
- Aleksandrov IN
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- Zhemchugov A
- Zheng J
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
- …